Optical waveguide modulator

ABSTRACT

A dual-differential optical modulator includes two optical waveguide arms, each including one or more phase modulating p/n junctions. The p/n junctions in each waveguide arm are electrically coupled between a same pair of single-ended transmission lines so as to be differentially push-pull modulated when the transmission line pair is connected to a differential driver. Either cathode or anode electrodes of the p/n junctions are AC coupled to the transmission lines and DC biased independently on the transmission line signals.

TECHNICAL FIELD

The present invention generally relates to optical modulators, and moreparticularly relates to a broad-band Mach-Zehnder optical waveguidemodulator configured for dual-differential driving using a singledifferential transmission line.

BACKGROUND

Broad-band optical communications typically require high-speedelectro-optical modulators (EOM) to modulate light at a desired datarate. One common type of a broad-band EOM is a Mach-Zehnder modulator(MZM) that uses a waveguide Mach-Zehnder (MZ) interferometric structurewith RF-driven optical phase modulators in each arm. The waveguide armsof the MZM are typically formed in an electro-optic material, forexample a suitable semiconductor or electro-optic dielectric materialsuch as LiNbO₃, where optical properties of the waveguide may becontrolled by applying a voltage to it. Such a waveguide modulator maybe implemented in an opto-electronic chip as a photonic integratedcircuit (PIC). A silicon photonics (SiP) platform based on Silicon onInsulator (SOI) technology may be particularly attractive forimplementing broad-band modulators as it enables a natural integrationwith CMOS-based high-speed electronic drivers.

One common technique to high-speed modulation of propagating light, inparticular at modulation rates on the order of 10-20 Gigabit per second(Gb/s) and higher, is the travelling wave approach, when the modulatingelectrical RF signals are applied to properly terminated electricaltransmission lines that are electro-optically coupled andvelocity-matched to the optical waveguides of the EOM. FIG. 1Aschematically illustrates an example broad-band EOM in the form of anMZM 10 with two optical waveguide arms 11, 12 coupled to two electricaldifferential transmission lines 30 of length L, each formed by an innersignal electrode 22 and an outer signal electrode 21, with correspondingground electrodes (not shown) and a differential transmission linetermination 25. In the SiP platform, the electrodes 21, 22 may beoverlaying p/n junctions formed across the waveguide arms that mayeither inject carriers (forward bias) or deplete carriers (reverse bias)in the waveguide core to modulate the refractive index of the waveguideby means of the carrier plasma dispersion effect. One known approach isa dual-differential modulation, in which each differential transmissionline (TL) 30 is driven with a differential RF signal, so that in eachdifferential TL 30 the inner electrode 22 and outer electrode 21 aredriven with complementary single-ended RF signals, and the p/n junctions31 in the waveguide arms 11, 12 are modulated in counter-phase; thiseffectively doubles the phase modulation amplitude at the output opticalcombiner of the MZM for a given peak-to-peak (PP) drive voltage Vppapplied to each electrode, as compared to more traditionalimplementations in which the inner electrodes 22 are grounded. The TLpairs 30 are configured so that the differential RF signals propagatealong them at the same velocity as the light that is travelling in thewaveguide arms 11, 12. In one common implementation, the PN junctions 31formed along the length of the TL pairs 30 are reverse-biased, and maybe referred to as depletion-mode high-speed phase modulators (HSPMs).However the dual differential modulator of the type illustrated in FIG.1A may require two differential drivers, or a single differential driverof a double output power, to drive the two electrode pairs 30, whichcomplicates the design. Additionally, further lessening the MZM driverpower requirements is desirable in many applications.

Accordingly, it may be understood that there may be significant problemsand shortcomings associated with current solutions and technologies forproviding high-bandwidth optical waveguide modulators.

SUMMARY

The present disclosure relates to an optical waveguide modulatorcomprising two waveguide arms and two single-ended transmission lines,wherein each of the waveguide arms is electrically coupled to each ofthe two single-ended transmission lines so as to be differentiallymodulated when complementary modulation signals are transmitted by thetwo single-ended transmission lines.

An aspect of the present disclosure provides an optical waveguidemodulator comprising: an input optical port for receiving input light;an output optical port for outputting modulated light; first and secondwaveguide arms extending optically in parallel between the input andoutput optical ports to guide the input light from the input opticalport to the output optical port along two light paths; a plurality ofp/n junctions comprising one or more first p/n junctions formed in thefirst waveguide arm one or more second p/n junctions formed in thesecond waveguide arm, each p/n junction comprising an anode electrodeand a cathode electrode. The optical waveguide modulator furthercomprises a first transmission line (TL) and a second TL, each extendingalong the first and second waveguide arms, wherein the first TL iselectrically coupled to the anode electrode of each of the one or morefirst p/n junctions and to the cathode electrode of each of the one ormore second p/n junctions, and the second TL is electrically coupled tothe cathode electrode of each of the one or more first p/n junctions andto the anode electrode of each of the one or more second p/n junctions.

According to an aspect of the present disclosure, each of the anodeelectrodes and/or each of the cathode electrodes of the first and secondp/n junctions is AC-coupled to one of the first and second TLs.

According to an aspect of the present disclosure, the optical waveguidemodulator may further include electrical circuitry for providing a DCbias voltage to at least one of the cathode and anode electrodes of eachp/n junction.

According to an aspect of the present disclosure, the optical waveguidemodulator may further include a differential driver configured to feedcomplementary electrical signals into the first and second transmissionlines. In some implementations the differential driver may be DC coupledto the first and second TLs. In some implementations the differentialdriver may include an open-collector differential amplifier stage thatis DC coupled to the first and second TLs.

In some implementations the electrical circuitry may include one or moreresistors electrically connected to the cathode electrodes for DCbiasing thereof.

In some implementations each of the anode electrodes may be AC-coupledto one of the first and second transmission lines, and each of thecathode electrodes is either DC-coupled or AC coupled to one of thefirst and second transmission lines.

In some implementations the electrical circuitry may include one or morecoupling electrodes electrically connected to the cathode electrodes orthe anode electrodes and capacitively coupled to one of the first andsecond transmission lines. In some implementations the one or morecoupling electrodes may be disposed over or under the first or secondtransmission lines with an insulating layer therebetween. In someimplementations the one or more coupling electrodes are disposed next tothe first or second transmission lines coplanar therewith.

In some implementations the first and second transmission lines maycross each other at least once forming a TL crossing. In someimplementations the one or more first p/n junctions comprises two firstp/n junctions of opposite polarity disposed at opposite sides of the TLcrossing, and the one or more second p/n junctions comprises two secondp/n junctions of opposite polarity disposed at opposite sides of the TLcrossing.

In some implementations one of the one or more coupling electrodesextends along the first TL for at least a portion of a length thereof,and at least one of the cathode electrodes or the anode electrodes iselectrically connected to the one of the one or more coupling electrodesat a distal end thereof that is farther away from an input end of thefirst TL for receiving an electrical drive signal.

An aspect of the present disclosure provides an optical waveguidemodulator comprising: an input optical port for receiving input light;an output optical port for outputting modulated light; first and secondwaveguide arms extending optically in parallel between the input andoutput optical ports to guide the input light from the input opticalport to the output optical port along two light paths; a first phasemodulator (PM) disposed in the first waveguide arm and comprising ananode electrode and a cathode electrode; a second PM disposed in thesecond waveguide arm and comprising an anode electrode and a cathodeelectrode, wherein each of the first and second PM is configured tomodulate a phase of light propagating therein in response to a voltageapplied between the anode and cathode electrodes thereof; a firsttransmission line (TL) extending along the first and second waveguidearms and electrically coupled to the anode electrode of the first PM andthe cathode electrode of the second PM; and, a second TL extending alongthe first and second waveguide arms and electrically coupled to thecathode electrode of the first PM and to the anode electrode of thesecond PM.

In some implementations the first and second waveguide arms may compriseelectro-optic material. In some implementations the first and secondwaveguide arms may comprise semiconductor material, and the first andsecond PMs may each comprise a p/n junction.

In some implementations at least the anode electrodes of the first andsecond PMs or at least the cathode electrodes of the first and secondPMs are AC-coupled to the corresponding first or second TLs.

In some implementations the waveguide modulator may comprise a siliconphotonics chip wherein the first and second waveguide arms and the firstand second TLs are formed, and wherein the semiconductor materialcomprised silicon.

In some implementations the waveguide modulator may include first andsecond coupling electrodes disposed next to the first and second TLsrespectively so as to be electrically AC coupled therewith, whereineither the anode electrodes or the cathode electrodes of the first andsecond PMs are electrically connected in DC to the first and secondcoupling electrodes respectively. In some implementations the first andsecond coupling electrodes may be disposed directly over or under thefirst and second TLs respectively.

An aspect of the present disclosure provides an optical waveguidemodulator comprising: two optical ports, an optical waveguide connectingthe two optical ports, two transmission lines (TLs) extending along alength of the optical waveguide, and, a plurality of phase modulators(PM) spread along the length of the optical waveguide, each PMelectrically connected to the two TLs and configured to modulate a phaseof light propagating in the optical waveguide in response to adifference in electrical signals propagating in the two TLs. The two TLsintersect at one or more locations to form one or more TL crossingswherein the TLs are magnetically coupled for increasing an effectiveinductance and an impedance thereof.

BRIEF DESCRIPTION OF THE DRAWINGS

Embodiments disclosed herein will be described in greater detail withreference to the accompanying drawings which represent preferredembodiments thereof, in which like elements are indicated with likereference numerals, and wherein:

FIG. 1A is a schematic block diagram of a travelling-wave waveguideMach-Zehnder modulator with a dual-differential modulation, in whicheach of the waveguides arms is differentially modulated using a separatepair of single-ended electrical transmission lines (TLs);

FIG. 1B is a schematic block diagram of a travelling-wave waveguideMach-Zehnder modulator with a single-differential modulation, in whicheach of the waveguides arms is modulated using a single-ended TL;

FIG. 2 is a schematic diagram of an optical dual differential modulator(DDM) in which HSPMs in both waveguides arms are differentiallymodulated using a same pair of single-ended electrical transmissionlines (TLs);

FIG. 3 is a schematic expanded view of a portion of an embodiment of themodulator of FIG. 2 with a modulating p/n junction in each waveguidearm;

FIG. 4A is a simplified electrical circuit diagram of an embodiment ofthe DDM of FIG. 2 with AC-coupled anodes of the HSPMs;

FIG. 4B is a simplified electrical circuit diagram of an embodiment ofthe DDM of FIG. 2 with AC-coupled cathodes of the HSPMs;

FIG. 5A is a schematic diagram of an embodiment of the DDM of FIG. 2with the cathodes of the HSPMs in each waveguide arm AC coupled to oneof the TLs by means of a common coupling electrode, and are separatelyDC biased;

FIG. 5B is a schematic diagram of a variation of the DDM of FIG. 5Aincluding a bias resistor for providing a DC bias voltage to thecoupling electrode for DC biasing the cathodes of the HSPMs connectedthereto;

FIG. 5C is a schematic diagram of an embodiment of the DDM of FIG. 5A inwhich the cathodes of the HSPMs in each waveguide arm are separately ACcoupled to one of the TLs and DC biased;

FIG. 6 is a schematic cross-sectional view of a DDM chip with ACcoupling electrodes with the cross-section taken in a lateral plane thatis normal to the direction of signal propagation in the device;

FIG. 7A is a schematic diagram illustrating a 3D view of an AC couplingbetween an HSPM and a TL using a separate MiM structure formed next tothe TL;

FIG. 7B is a schematic diagram illustrating a 3D view of an AC couplingbetween an HSPM and a TL using a separate MiM structure formed directlybelow the TL;

FIG. 7C is a schematic diagram illustrating a 3D view of an AC couplingbetween an HSPM and a TL using a coupling electrode disposed under theTL and forming a MiM structure therewith;

FIG. 7D is a schematic diagram illustrating a 3D view of a variation ofthe AC coupling structure of FIG. 7C with the HSPM connected to thecoupling electrode at a distal end thereof in the direction of RF signalpropagation;

FIG. 8A is a simplified electrical circuit diagram of an embodiment of aDDM with the HSPNs connected to distal ends of MiM structures thatprovide the AC coupling between the TLs and the HSPMs;

FIG. 8B is a simplified electrical circuit diagram of an embodiment of aDDM with the HSPNs connected to distal ends of coupling electrodes thatprovide the AC coupling between the TLs and the HSPMs;

FIG. 9 is a schematic diagram of an embodiment of a DDM with two TLscrisscrossing for enhanced magnetic coupling therebetween;

FIG. 10 is a schematic diagram of an embodiment of a DDM with two TLsrouted to include overlapping loops for enhanced magnetic couplingtherebetween;

FIG. 11 is a schematic diagram of a portion of a travelling wave opticalmodulator with two TLs routed to form one or more TL crossings;

FIG. 12A is a diagram illustrating bias circuitry of a DDM with an opencollector driver and simultaneous biasing of HSPMs and the driverthrough TL termination resisotrs;

FIG. 12B is a diagram illustrating bias circuitry of a DDM with an opencollector driver and simultaneous biasing of HSPMs and the driver usinga bias-T;

FIG. 13 is a schematic plan view of an electrical layout of a portion ofa DDM chip in one implementation thereof;

FIG. 14 is a zoomed-in view of the electrical layout of a modulatingsegment of the DDM chip of FIG. 13.

DETAILED DESCRIPTION

In the following description, for purposes of explanation and notlimitation, specific details are set forth, such as particular circuits,circuit components, techniques, etc. in order to provide a thoroughunderstanding of the present invention. However, it will be apparent toone skilled in the art that the present invention may be practiced inother embodiments that depart from these specific details. In otherinstances, detailed descriptions of well-known methods, devices, andcircuits are omitted so as not to obscure the description of the exampleembodiments. All statements herein reciting principles, aspects, andembodiments of the invention, as well as specific examples thereof, areintended to encompass both structural and functional equivalentsthereof. Additionally, it is intended that such equivalents include bothcurrently known equivalents as well as equivalents developed in thefuture, i.e., any elements developed that perform the same function,regardless of structure.

Furthermore, the following abbreviations and acronyms may be used in thepresent document:

CMOS Complementary Metal-Oxide-Semiconductor

BiCMOS Bipolar CMOS

GaAs Gallium Arsenide

InP Indium Phosphide

LiNbO3 Lithium Niobate

PIC Photonic Integrated Circuits

SOI Silicon on Insulator

SiP Silicon Photonics

PSK Phase Shift Keying

BPSK Binary Phase Shift Keying

QAM Quadrature Amplitude Modulation

QPSK Quaternary Phase Shift Keying

RF Radio Frequency

DC Direct Current

AC Alternate Current

OSNR Optical Signal to Noise Ratio

MiM Metal-Insulator-Metal

RMS Root Mean Square

Note that as used herein, the terms “first”, “second” and so forth arenot intended to imply sequential ordering, but rather are intended todistinguish one element from another, unless explicitly stated.Similarly, sequential ordering of method steps does not imply asequential order of their execution, unless explicitly stated. The word‘using’, when used in a description of a method or process performed byan optical device such as a polarizer or a waveguide, is to beunderstood as referring to an action performed by the optical deviceitself or by a component thereof rather than by an external agent.Notation Vπ refers to a bias voltage of a Mach-Zehnder modulator (MZM)that corresponds to a change in a relative phase delay between arms ofthe MZM by π radian (rad), or 180 degrees, which corresponds to a changefrom a minimum to a next maximum in the MZM transmission versus voltage.Radio frequency (RF) may refer to any frequency in the range fromkilohertz (kHz) to hundreds of gigahertz (GHz). The term p/n junctionencompasses p/i/n junctions having a region of substantially intrinsicconductivity located between the p-doped and n-doped regions. The term“differential signal” refers to a signal composed of two single-endedsignals having complementary AC components. The term “inverteddifferential signal” refers to a differential signal having ACcomponents of its constituent single-ended signals inverted relative tothose of a reference differential signal, or a differential signalhaving high-low and low-high transitions switched. The term“transmission line” (TL) may be used herein to refer to a signalelectrode of a transmission line, with the understanding that at leastone ground electrode may also present. The term “single-endedtransmission line”, or “single-ended TL”, refers to a TL that includes asingle signal electrode along which a single-ended RF signal maypropagate. The term “differential transmission line”, or “differentialTL”, refers to a TL that includes a pair of signal electrodes alongwhich two complementary single-ended RF signals may propagate. The term“electrically connected” is used herein to mean a DC electricalconnection with a conducting pathway, unless explicitly statedotherwise. The term “AC coupled” is used herein to mean anelectromagnetic, such as capacitive and/or inductive, coupling betweentwo or more elements in the absence of a DC electrical connectionbetween the elements, unless explicitly stated otherwise. The term“electrically coupled” encompasses both DC and AC electrical coupling.

The present disclosure relates to an electro-optic modulator (EOM) and arelated method in which two optical waveguides, also referred to hereinas the waveguide arms, are used to guide input light from an inputoptical port to an output optical port along two or more optical paths;such EOMs may also be referred to herein as an optical waveguidemodulator or as an optical modulator. One aspect of the presentdisclosure relates to a dual-differential EOM, which is also referred toherein as the dual-differential modulator (DDM), wherein each of the twowaveguide arms is differentially modulated, i.e. modulated by adifferential RF signal, and wherein the modulating differential signalis provided to each of the waveguide arms from the same two transmissionlines (TLs); thus both waveguide arms may be modulated using the samedifferential amplifier that drives a single TL pair, which reduces thepower requirements on the differential driver up to a factor of twocompared to the DDM 10 of FIG. 1A in which each waveguide arm is drivenby a dedicated TL pair.

In order to better understand advantages of this approach, it may beinstructive to first consider the DDM 10 illustrated in FIG. 1A, inwhich two TL pairs 30 are used to drive two sets of depletion-mode HPSMs31, each set disposed to modulate one of the waveguide arms 11 and 12.Typically, a MZM requires a relatively large modulation voltage swing(>5V), which is provided by the modulator driver 35. Broad-bandmodulation requires the use of high-speed transistors in the modulatordriver. However, transistors designed for high-speed operation have arelatively low breakdown voltages, which limits the driver maximumoutput voltage swing. Reliability and lifetime of the driver'stransistors are compromised when driving voltages exceed their breakdownlimits. The trade-off between speed and maximum output voltage swinglimits the performance of the driver implemented in a given technology.

Another issue of practical importance that is related to the driver'smaximum voltage swing is the power consumption, which reduction istypically desired. The part of the RF power P_(diss) dissipated in theMZM that depends on the voltage swing at the driver's output isinversely proportional to the characteristic impedance Z_(MOD) of themodulator, P_(diss)=V_(RMS_SWING) ²/Z_(MOD), where V_(RMS_SWING) is theRMS value of the peak-to-peak voltage swing V_(PP) at the output of thedriver, for example for a sinusoidal signal V_(RMS_SWING)=V_(PP)/2˜2).Thus, increasing the modulator impedance Z_(MOD) allows to reduce itspower consumption, and ultimately the cost of manufacturing andoperating the optical transmitter. Furthermore, replacing two TL pairswith one allows to reduce the modulator food print and thus the chiparea of the modulator. Furthermore the increase in modulator impedancemay be used in a tradeoff with other design parameters of the modulator,for example by “trading” the increase in the impedance for a higherbandwidth.

For the DDM 10, the modulator impedance Z_(MOD) is the load impedanceZ_(DDM) of the differential driver 35, which is defined by the impedanceof the two TL pairs 30 connected in parallel, i.e. Z_(DDM)=Z/2. HereZ=sqrt(L_(TL)/(C_(TL)+C_(HSPM))) is the impedance of each TL pair 30,with L_(TL) and C_(TL) denoting the inductance and capacitance of one TLpair 30, respectively, and C_(HSPM) is the total capacitance of theHSPMs in one waveguide arm.

The DDM of the type illustrated in FIG. 1A, in which two TL pairs 30 aredriven in parallel by a single differential driver 35, requires half ofa voltage swing of a single-differential modulator (SDM) of FIG. 1B, inwhich e.g. inner electrodes 22 of each TL pair 30 are grounded and theouter electrodes 21 are differentially driven, as illustrated in FIG.1B. However, since in the embodiment of FIG. 1A the differential driver35 feeds into two TL pairs 30 in parallel, it has to provide twice thecurrent of an SDM driver 36 of FIG. 1B. Therefore drivers of equivalentDDM and SDM may consume about the same amount of power, and the reducedvoltage swing of the DDM of FIG. 1A, as compared to an equivalent SDM ofFIG. 1B, is obtained at the cost of increased complexity and chip area.

Turning now to FIG. 2, there is schematically illustrated an improvedDDM 100 in accordance with an example embodiment of the presentdisclosure, in which power and/or chip area requirements areadvantageously relaxed. In the illustrated embodiment, HSPMs disposed ineach of two waveguide arms 111, 112 of a Mach-Zehnder interferometer(MZI) 110 are differentially driven by complementary RF signals 151, 152from the same two single-ended TLs 111, 112 that extend along thewaveguide arms 111, 112 and are fed at their input ends from adifferential RF driver 135. Since each of the waveguide arms 111, 112 ofthe MZI 110 is differentially modulated, the peak-to-peak voltage swingV_(PP) that driver 135 needs to generate is one half of that of anequivalent SDM. Furthermore since driver 135 has to drive only a singlepair of TLs 131, 132, its load impedance may be substantially equal tothe load impedance of an equivalent SDM and is twice the load impedanceof the DDM of FIG. 1A, thereby advantageously reducing the powerrequirements on driver 135.

Continuing to refer to FIG. 2, in the illustrated embodiment DDM 100includes an input optical port 141 for receiving input light 101, anoutput optical port 142 for outputting modulated light 103, and firstand second waveguide arms 111, 112 extending optically in parallelbetween the input and output optical ports 141, 142 to guide the inputlight 101 from the input optical port 141 to the output optical port 142along two light paths. The first waveguide arm 111 includes one or morefirst HSPMs 121 ₁, 121 ₂, . . . 121 _(n) that may be referred generallyas the first HSPMs 121, while the second waveguide arm 112 includes oneor more second HSPMs 122 ₁, 122 ₂, . . . 122 _(n) that may be referredgenerally as the second HSPMs 122. The number n of the HSPMs in eachwaveguide arm 111, 112 may vary from 1 to 20 or more, and may be thesame for each waveguide arm, although it is not a requirement. Inexample embodiments described hereinbelow each of the first and secondHSPMs 121, 122 has two electrodes, which are disposed at opposite sidesof the respective waveguide arm, and which may be referred to herein asthe anode electrode and the cathode electrode, or simply the anode andthe cathode. The HSPMs 121, 122 are configured to vary the refractiveindex in at least a portion of the respective waveguide arm independence to a sign and magnitude of a voltage applied between theanode and the cathodes electrodes, thereby modulating the optical phaseof light propagating therethrough. In some embodiments the HSPMs 121,122 may be configured so that their phase modulation efficiency dependson the location along the waveguide arms 111, 112. Although the firstand second HSPMs 121, 122 are shown in FIG. 2 with a relative shifttherebetween along the length of the DDM for convenience ofillustration, in a typical embodiment they may be pair-wise aligned soas to be at a same optical distance from an input optical port 141.

Referring also to FIG. 3 that schematically illustrates a portion of theDDM 100 including one HSPM 121 and one HSPM 122, in example embodimentsdescribed hereinbelow each of the HSPMs 121 and 122 may be in the formof a p/n junction with an anode electrode 121 a or 122 a respectively,and a cathode electrode 121 k or 122 k respectively. In such embodimentsthe first HSPMs 121 may also be referred to as the first p/n junctions121, and the second HSPMs 122 may also be referred to as the second p/njunctions 122.

In one embodiment one of the TLs 121, 122, for example the first TL 131may be electrically coupled to the anode electrode 121 a of each of theone or more first HSPMs 121 and to the cathode electrode 122 k of eachof the one or more second HSPMs 122, and the other of the two TLs, forexample the second TL 132 may be electrically coupled to the cathodeelectrode 121 k of each of the one or more first HSPMs 121 and to theanode electrode 121 a of each of the one or more second HSPMs 122. Withthis configuration, when the first and second TLs are differentiallydriven with complementary single-ended signals 151, 152, the first andsecond HSPMs 121, 122 are modulated in counter-phase, thereby affectinga push-pull modulation of light in the first and second waveguide arms111, 112.

The first and second TLs 111 and 112 are represented in FIG. 2 by theirrespective signal electrodes but may also include one or more groundelectrodes that are not shown in the figure to avoid clutter. They maybe generally in the form of any suitable TLs, including but not limitedto microstrip TL, coplanar (CPW) TL, conductor backed CPW, and striplineTL. The first and second TLs 111 and 112 are differentially driven fromone end by differential driver 135 and are terminated at the other endswith a suitable line termination 113, which may be in the form orinclude a resistor, having a characteristic impedance Z_(DDM2)/2 so asto suppress the reflection of electrical signals at the end of the TL.Here Z_(DDM2) denotes the load impedance seen by the differential driver135:

$Z_{{DDM}\; 2} = \sqrt{\frac{L_{DTL}}{C_{HSPM} + C_{DTL}}}$

where L_(DTL) and C_(DTL) are the inductance and capacitance of thedifferential TL formed by the first and second single-ended TLs 131,132, and C_(HSPM) is the total capacitance of all HSPMs 121 and 122 inboth waveguide arms 111, 112. The load impedance Z_(DDM2) seen by driver135 is greater than the load impedance seen by driver 35 of the DDM ofFIG. 1, DDM 100 requires less current, and therefore lower power, toachieve the same modulation efficiency of the input light 101.

In one embodiment the waveguides of the MZI 110 and the signalelectrodes 111, 112 may be formed in a semiconductor chip, such as forexample a silicon photonics (SiP) chip, GaAs based chip, or InP basedchip, or any other chip of a suitable semiconductor material. In oneembodiment the MZI 110 and TLs 131, 132 are formed in or upon a SOIchip, with the waveguides forming the MZI 110 having their cores definedin a silicon layer of the SOI chip. In one embodiments HSPMs 121 and 122may be depletion-type HSPMs in the form of p/n junctions, for exampleformed within the Si waveguide cores. In some embodiment the p/njunctions 121, 122 may be in the form of PIN junctions, with anintrinsic (I) region in the middle of the waveguide core sandwichedbetween a P-doped and an N-doped regions. It will be appreciated that awaveguide MZI with p/n junction based HSPMs in its arms may also beformed in semiconductor materials other than Si, and correspondingembodiments of the DDM 100 are within the scope of the presentdisclosure.

When embodied as p/n junctions, the HSPMs 121, 122 modulate therefractive index in the waveguide arms 111, 112 by varying theconcentration of free charge carriers therein in response to an appliedvoltage, thereby modulating an optical phase of light propagating in thewaveguides. For optimal operation the p/n junctions 121, 122 may besuitably biased, for example reversed biased so as to operate in thedepletion mode in which the number of free carriers in the waveguide isrelatively small. When reverse biased, the p/n junctions 121, 122 may bereferred to as carrier depletion based HSPMs. Accordingly, in suchembodiments DDM 100 may include electrical circuitry for providing a DCbias voltage to at least one of the cathode and anode electrodes of eachp/n junction 121 and 122. In some embodiments it may be configured toprovide different DC voltages to the anodes and the cathodes of the p/njunctions 121, 122 independently on the RF data signals 151, 152propagating along the TLs 131, 132. This circuitry may include biasresistors, electrical leads, and circuitry providing AC couplingpathways between the cathodes 121 k, 122 k of the p/n junctions 121, 122and the TLs 131, 132 and/or AC coupling pathways between the anodes 121a, 122 a of the p/n junctions 121, 122 and the TLs 131, 132.

FIGS. 4A and 4B illustrate simplified electrical circuit diagrams of asection of the DDM 100 encompassing two HSPMs in each waveguide arm (notshown) for two example embodiments. Turning first to FIG. 4A, in thisembodiment the cathodes of the p/n junctions 121 and 122, which areshown as diodes, are DC coupled to the signal electrodes of the TLs 131and 132, respectively, while the anodes of all the p/n junctions 121,122 are AC-coupled to the corresponding TLs, as indicated by capacitors128 representing the effective capacitance of the corresponding ACcoupling structures. The anode bias voltage Va is supplied to the anodesof the p/n junctions 121, 122 via dedicated bias resistors R_(H), whilethe cathode bias voltage Vk is supplied to the cathodes of the p/njunctions via a bias resistors R_(L) and the signal electrodes of theTLs 121, 122. In the embodiment illustrated in FIG. 4B the polarity ofeach of the p/n junctions 121, 122 is flipped, so that the anodes of thep/n junctions 121 and 122 are DC coupled to the signal electrodes of theTLs 131 and 132 to receive the anode bias voltage Va that is provided tothe TLs via the bias resistor R_(L). The cathodes of all the p/njunctions 121, 122 in this embodiment are AC-coupled to the signalelectrodes of the corresponding TLs, and receive the cathode biasvoltage Vk via the dedicated bias resistors R_(H). It will beappreciated that in other embodiment both the cathode electrodes and theanode electrodes of each, or at least some, of the p/n junctions 121,122 may be AC coupled to the signal electrodes of the TLs 131, 132.Resistors R_(L) may be selected so as to provide the desired TLtermination 113 as illustrated in FIG. 2. Resistors R_(H) defines thelow-cutoff frequency f_(c), =1/(2πR_(H)C_(AC)). Each of the resistorsR_(H) and R_(L) may be for example in the range of tens of ohms andkiloohms to megaohms. The effective capacitance C_(AC) of theTL-anode/cathode AC coupling, represented by the capacitors 128, may befor example in the range of tens of femtofarads to units of picofarads.

Turning now to FIG. 5A, there is schematically illustrated a plan viewof an example embodiment of DDM 100 in which the cathodes of p/njunctions 121, 122 are AC coupled to the TLs 131, and 132, respectively,by means of coupling electrodes 161 and 162 that are disposed next tothe corresponding TLs 131, 132 but without a direct electrical contacttherebetween. The cathodes of the p/n junctions 121 are electricallyconnected, for example by suitable low-resistance conducting pathways215, to the coupling electrode 162 that is AC coupled to TL 132, whilecathodes of the p/n junctions 122 are electrically connected, forexample by suitable low-resistance conducting pathways 216, to thecoupling electrode 161 which is AC coupled to TL 131. In the illustratedembodiment the coupling electrodes 161 and 162 are disposed directlyunder TLs 131 and 132, respectively, although in other embodiments theymay be disposed over or next to the respective TLs, with a thininsulating layer or material therebetween, so as to provide the desiredAC coupling to the signal electrode of the respective TL whileinsulating the cathodes therefrom in DC. In the illustrated embodimentthe anodes of the HSPMs 121, 122 are DC coupled to the respective TLs.Cathode biasing resistors 221 for individually DC biasing the cathodesof each of the p/n junctions 121, 122 may be implemented in the samechip as the MMZ 110 and the TLs 131, 132, or they may be a part of anexternal biasing circuit. It will be appreciated that the polarities ofthe HSPMs 121, 122 may be flipped, so that the anodes are AC coupled andthe cathodes are DC coupled as illustrated in FIG. 4B.

In the embodiment of FIG. 5A each of the HSPMs' 121 cathodes is ACcoupled to TL 132 through a same coupling electrode 162 and DC biasedfrom a dedicated resistor 221, while each of the HSPMs' 122 cathodes isAC coupled to TL 131 through a same coupling electrode 161 and DC biasedfrom its own dedicated resistor 221. In other embodiments the DC cathodebias voltage Vk may be applied through each of the coupling electrodes161, 162, as illustrated in FIG. 5B. In yet another embodimentillustrated in FIG. 5C, the cathodes or anodes of each of the HSPMs 121and 122 may each use a separate AC coupling arrangement 171, e.g. in theform of a separate coupling electrode, for coupling to the respectiveTL. It will be appreciated that the polarity of the HSPMs 121, 122 inFIGS. 5A-5C may be flipped so that it is the HSPM anodes that are ACcoupled to the respective TLs, or the structure modified so that boththe cathodes and the anodes of the HSPMs 121, 122 are AC coupled to therespective TLs.

Referring to FIG. 6, it schematically illustrates a lateralcross-section of a chip implementing the DDM 100 in an exampleembodiment thereof. The cross-section is taken across the devicestructure perpendicularly to the direction of light propagation in theDDM. It will be appreciated that the view illustrated in FIG. 6 is byway of illustration only, and the chip may include also other layersand/or elements that are not shown in the figure. In the illustratedexample embodiment the waveguide arms 111 and 112 are shown disposedover a support substrate or wafer 199 in an insulating cladding layer ormaterial 165. Coupling electrodes 161, 162 are disposed directly underthe signal electrodes of TLs 131, 132, so as to provide the AC couplingthereto. The thickness of the intermediate insulating layer 165 betweenthe coupling electrodes 161 and 162 and the corresponding signalelectrodes of TLs 131 and 132 may be for example, in the range of 0.1 μmto 1 μm, or as needed to obtain the desired AC coupling and DCinsulation between the respective electrode pairs 131-161 and 132-162.Ground electrodes 135 may be disposed coplanar with the signalelectrodes of the TLs 131, 132 as illustrated by way of example, but mayalso be provided in a different plane, for example on the back side ofsubstrate 199. In one embodiment substrate or wafer 199 may be forexample a silicon substrate, the insulating material 165 being forexample silicon dioxide, with silicon waveguides 111, 112, and metalelectrodes 131, 132, 161, 162, 135.

Turning now to FIGS. 7A-7D, the AC coupling between the HSPM cathodes oranodes and the corresponding TLs may be arranged in a variety of ways,for example using metal-insulator-metal (MiM) structures such as thoseschematically illustrated in the figures. Referring first to FIG. 7A, aTL signal electrode 331, which may for example represent the signalelectrode of either TL 131 or 132 of DDM 100, is electrically connected,for example using a metallic conductor, to one of two metal electrodesof a MiM structure 328, with the anode of an HSPM 321, schematicallyillustrated by a diode symbol, electrically connected to the otherelectrode of the MiM structure 328. HSPM 321 may represent either HSPM121 or 122 of DDM 100. The MiM structure 328 is designed to provide thedesired AC coupling between the TL signal electrode 331 and the HPSM321. Substrate 399 supports the TL 331, MiM 328 and HSPM 321. There is aparasitic capacitive coupling between each of TL 331, MIM 328 andsubstrate 399, which may negatively affect the device performance. Thisparasitic capacitive coupling may be somewhat reduced by disposing MiM328 directly beneath the signal electrode of TL 331, as illustrated inFIG. 7B, so that MiM 328 at least partially shields TL 331 fromsubstrate 399. Turning now to FIG. 7C, the TL-HSPM AC coupling may besimplified, and the parasitic coupling to the substrate further somewhatreduced, by replacing a separate MiM structure 328 with a couplingelectrode 361 that forms a MiM structure directly with the signal TLelectrode 331.

Continuing to refer to FIGS. 7A-7D, MiM 328 or coupling electrode 361may extend along at least a portion of a length of TL 331, with theanode of HSPM 121, or in another embodiment the cathode thereof,electrically connecting to a corresponding AC coupling electrode at anypoint along its length. Advantageously, they provide additional ACloading of the TL 331 that somewhat increases the device' impedance asseen by the DDM driver. This AC loading may have both a capacitive andan inductive components. In embodiments wherein the length L_(MiM) ofthe corresponding MiM structure, for example the length of the couplingelectrode 361, is comparable or exceeds the wavelength of the modulatingRF signal propagating along TL 331, this AC loading may be furtherincreased by connecting HSPM 321 to the MiM, e.g. the coupling electrode361, at a distal end thereof that is farther away from the input end ofthe TL 331, as illustrated in FIG. 7D. This increases the inductance ofthe MiM structure and thus the AC loading of the TLs, which serves toincrease the device impedance, and thus may lessen the driver powerrequirements.

FIGS. 8A and 8B schematically illustrate electrical circuitry of twoexample implementations of a DDM using MiM structures of the typeillustrated in FIGS. 7A and 7C, respectively, configured for enhancedinductive contribution to the device impedance. In FIG. 8A the ACcoupling between the HSPMs, illustrated with the diode symbols, and theTLs 331, 332 is provided by MiM structures 328, each of which extendsalong a length of a respective TL 331 or 332, with a distal endconnected to an HSPM. In FIG. 8A the cathodes of HSPMs, or the anodesthereof in other embodiments, connect to distal ends of couplingelectrodes 361 that are AC coupled to the respective TLs 331 or 332. Inboth figures the direction of the RF signal propagation is shown with anarrow labeled “RF”. The term ‘distal end’ means the end of a MiMstructure or an electrode that is farther away from the RF input end ofthe TLs.

In some embodiments the impedance of a DDM may be advantageouslyincreased by configuring the single-ended TLs of a differentially-drivenTL pair so as to increase their mutual inductance, for example shapingor routing them so that the TLs cross each other in one or more pointsthereby facilitating a magnetic coupling between the TLs.

Referring now to FIG. 9, an example DDM 400 is schematically illustratedin which two TLs 431, 432 meander so as to cross each other at aplurality of locations along the length of the device. Similarly to theDDMs described hereinabove with reference to FIGS. 2, 5A-5C, DDM 400includes MZI 110 with a set of first HSPMs 421 formed in its firstwaveguide arm 111 and a set of second HSPMs 422 formed in its secondwaveguide arm 112, where the number N of HSPMs in each waveguide arm canvary from 2 to 20 or more depending on implementation, with N=4illustrated in the figure by way of example. Each of the HSPMs 421, 422is differentially driven by complementary RF signals propagating alongtwo single-ended TLs 431, 432, and are coupled to the TLs so thatcorresponding HSPMs in the first and second waveguide arms 111, 112 aremodulated in counter-phase. In the illustrated embodiment the anode ofeach HSPMs 421 or, 422 is DC coupled to one of the TLs and is DC biasedtherefrom with a DC voltage Va that is applied to the TL via resistor442, while its cathode is AC coupled to the other of the two TLs and isDC biased with voltage Vk through a dedicated resistor 441. In otherembodiments the polarities of the HSPMs 421, 422 may be reversed, orboth the anodes and the cathodes may be AC coupled to the respectiveTLs. The TLs 431, 432 extend along the length of the device in acrisscross or meandering fashion, crossing each other at a plurality oflocations along the device's length. The illustrated embodiment includesfive TL crossings, but in other embodiments the number of crossing maybe different, generally one or greater. Mutual TL inductance at the TLcrossings due to the magnetic coupling between the TLs 431, 432 at thecrossings 455 increases the device impedance seen by the differentialdriver 435, thereby enabling lower driver power for a same voltage swingVpp. In order to facilitate push-pull modulation, two HSPMs disposed inthe same waveguide arm at opposite side of a TL crossing may be ofopposite polarity, so that for example the set of first HSPMs 421includes two first HSPMs 421 a, 421 b of opposite polarity disposed atopposite sides of a TL crossing 455, and the set of second HSPMs 422includes two second HSPMs 422 a, 422 b of opposite polarity disposed atopposite sides of the TL crossing 455.

It will be appreciated that FIG. 9 illustrates one of possibleembodiments of a DDM with TL crossings that enhance their effectiveinductance, and other embodiments can be envisioned. FIG. 10 illustratesanother example embodiment in which two TLs 531, 532, which drive twosets of HSPMs 521, 522 are routed to intersect at a plurality of devicelocations. In this example the TLs 531, 532 are routed to formoverlapping TL loops or contours 541, 542, in which RF signals 551, 552travel in opposite directions, thereby facilitating a strong magneticcoupling between the TLs at locations 501 of the loops. This strongmagnetic coupling increases mutual inductance of the TLs, and thusincreases the device's impedance as seen by a differential driverconnected at one end of the TLs (not shown). Although FIG. 10 shows theoverlapping TL loops at three locations 501 along the length of thedevice, with one pair of HSPMs 521, 522 therebetween, it will beappreciated that that is by way of example only, and in otherembodiments the number of such locations where the TLs loop, and/or thenumber of HPSMs pairs therebetween, may differ from what is shown inFIG. 10.

FIGS. 9 and 10 illustrate the use of TL crossings in DDMs in which twosets of HSPMs disposed in the two waveguide arms of an MZI are drivenfrom a single TL pair. However a TL routing that facilitates magneticcoupling of two differentially driven TLs may be advantageously used inother types of differentially-driven travelling wave optical modulators,including but not limited to MZI-based modulators and ring modulators,among others.

With reference to FIG. 11, there is schematically illustrated atravelling-wave optical waveguide modulator according to an embodimentof the present disclosure. The modulator includes an optical waveguide611 that may be connecting two optical ports 601, 602. A sequence ofphase modulators (PMs) 621 is disposed along a length 1 of the opticalwaveguide 611, each having two electrodes that connect to a first TL 631and a second TL 632. The TLs 631, 632 extend along the length 1 ofwaveguide 611 where the PMs 621 are located, and are routed to intersecteach other in one or more locations, forming one or more TL crossings.The PMs 621 may be configured to modulate a phase of light propagatingin waveguide 611 in response to a difference in electrical signalspropagating in the two TLs 631, 631. In one embodiment the PMs 621 maybe in the form of p/n junctions with at least one of the anode electrodeand the cathode electrode thereof AC coupled to one of the TLs 631, 632,for example as described hereinabove. In another embodiment the PMs 621may be based on a linear electro-optic effect (Pockels), such as thatexisting in lithium niobate (LiNbO3) and similar electro-opticmaterials. Although schematically shown as straight, waveguide 611 maybe curved in some embodiments. The modulator illustrated in FIG. 11 mayrepresent for example one waveguide arm, or a portion thereof, of adifferentially-driven travelling-wave MZI modulator. In otherembodiments it may represent another differentially-driventravelling-wave MZI modulator, or a portion thereof, for example aportion of a ring modulator. The TL crossing or crossings 655 facilitatemagnetic coupling between the TLs 631, 632 for increasing an effectiveinductance and an impedance thereof. Although TLs 621, 622 in FIG. 11meander to form a linear sequence of one or more TL crossings 655, twoin the concrete example shown, in other embodiments more complex routingof the TLs may be implemented, including but not limited to a TL routingwherein the two TLs form one or more overlapping loops along the lengthof the device, such as illustrated in FIG. 10.

FIGS. 12A and 12B illustrate example electrical biasing schemes of a DDMaccording to one or more embodiments of the present disclosure. In eachof the FIGS. 12A and 12B, two sets of HSPMs 621 and 622, which may besequentially disposed along two waveguide arms of an MZI for example asdescribed hereinabove with reference to FIGS. 2, 5A-5C, are electricallycoupled to a same pair of TLs 631, 632. The HPSMs 621, 622 may be eachin the form of a p/n junction including an anode electrode and a cathodeelectrode, one of which is AC coupled to one of the TLs and the othermay be either AC or DC coupled. In the illustrated examples the cathodesof the HSPMs 621, 622 are AC coupled to the TLs 631, 632, respectively,while the anodes of the HSPMs 621, 622 are DC coupled to the TLs 632,631, respectively. In each of the figures, the TLs 631, 632 are both DCcoupled to a modulator driver 635. In the illustrated embodiments themodulator driver 635 includes at its output a differential amplifierformed by two transistors connected in an open collector, or open drain,configuration, with their emitters (sources) commonly connected to acurrent source that in operation generates a bias current Ibms. Thecollector or drain of each transistor is DC coupled to one of the twoTLs 631, 632. Advantageously, with a driver in an open collectorconfiguration the electrical power dissipated by the driver is reducedbecause there is no need for a termination impedance at the modulatorinput.

In a further advantage, the DC coupling of the open collector driver 635to the TLs 631, 632 enables to bias the driver and one the cathode orthe anode electrodes of the HSPMs 621, 622 from a same bias voltagesource or sources through bias resistors R_(L). In the embodiment ofFIG. 12A, the TLs 631, 632 are biased from a same source of bias voltage611. In operation the bias voltage source 611 outputs bias voltageV_(bias)=Vk+I_(bias)·R_(L)/2, where I_(bias) is the current generated bythe driver current source. This sets the HSPM cathode voltage Vk, whichin the illustrated biasing scheme is also a bias voltage of the driver634. In one embodiment Vk, and thus the bias voltage V_(bias), may beselected to provide a desired operating point of the driver 635, withthe anode voltage Va of the HSPMs 621, 622 then selected relative to Vkto provide a desired operation point of the of the HSPMs 621, 622.

FIG. 12B illustrates a Bias-T biasing scheme, in which a bias voltage Vkis provided to the TLs 631, 632 from voltage sources 651, 652 viahigh-impedance inductors 641 and 642, respectively. The inductance L_(T)of each of the inductors 641, 642 may be selected high enough so thatthe impedance Z_(L)=j2πf·L_(T) of each inductor 641, 642 is much greaterthan R_(L), for example by a factor of 10 or more, at any givenfrequency f within the operating bandwidth of the modulator, so as toavoid impacting the transmitter performance. This biasing scheme using abias-T enables to set the cathode bias voltage and the driver biasvoltage to a desired voltage Vk using lower-voltage sources 651, 642 ofthe bias voltage, thereby providing a further power saving of(I_(bias))²·R_(L)/4.

With reference to FIG. 13, there is illustrated a portion of an exampleelectrical layout of a travelling-wave MZI-based DDM that may beimplemented in a silicon photonics chip. Optical waveguides 711, 712that form the two arms of the MZI may be implemented in a silicon layerof the chip, with one or more p/n junctions formed in each of thewaveguides along their length. The waveguides 731, 732 may have one ormore waveguide loops 640 spread along the length of the device toprovide velocity matching with the RF signals propagating along TLs 731and 732. The TLs 731 and 732 are represented in the figure by theirsignal electrodes, with two ground planes 730 completing the TLs. Twosets of HSPMs 721, 722 are formed along the waveguides, with each HSPMformed by providing anode and cathode electrodes in electrical contactswith the p-doped and n-doped regions of the p/n junction, respectively,at a target location along the waveguides.

Referring now also to FIG. 14, the modulating portion of the DDM of FIG.13 may be viewed as a sequence of modulator segments 750 having one HSPMin each waveguide arm; FIG. 14 shows an expanded view of one suchmodulator segment. Each of the HSPMs 721, 722 formed by a cathodeelectrode 761 and an anode electrode 762 of a p/n junction in arespective waveguide arm, with the cathode electrodes 761 AC coupled tothe respective TLs 731 or 732 with a MIM capacitor 755. Bias resistors711 connect the cathodes 761 to respective bias metal traces 711,insulated from the ground electrodes 730, for connecting to a DC voltagesupply. All elements illustrated in FIGS. 13, 14 may be formed in a sameSOI chip with a compact form factor using CMOS technology.

The above-described exemplary embodiments are intended to beillustrative in all respects, rather than restrictive, of the presentinvention. Indeed, various other embodiments and modifications to thepresent disclosure, in addition to those described herein, will beapparent to those of ordinary skill in the art from the foregoingdescription and accompanying drawings.

For example, it will be appreciated that different electro-opticdielectric materials and semiconductor materials other than silicon,including but not limited to compound semiconductor materials of groupscommonly referred to as A3B5 and A2B4, such as GaAs, InP, and theiralloys and compounds, as well as such electrooptical materials aslithium niobate (LiNbO3) and the like, may be used to fabricate theoptical modulator circuits example embodiments of which are describedhereinabove. In addition, phase modulators other than p/n junctions canbe used in semiconductor waveguides, including silicon waveguides, suchas for example capacitive devices, silicon-insulator-silicon modulatingstructures, etc. In some embodiments wherein DC biasing of the HSPMs isnot required, the HSPMs in each MZI arm may be DC coupled to the TLs. Inother embodiments, HSPMs in each MZI arm may be AC coupled to each TL.In another example, although in the example embodiments describedhereinabove the cathode and the anode electrodes of the HSPMs were DCbiased using resistors, such as resistors RH in FIGS. 4A and 4B andresistors 221 or 222 in FIGS. 5A-5C, in other embodiments some or all ofthose resistors may be omitted and the DC bias voltage Va or Vk suppliedusing a bias-T. In another example, instead of using the same resistorfor the TL termination 113 and to bias the HSPM electrodes that are DCcoupled to the corresponding TL, such as for example illustrated inFIGS. 4A-5C, different resistors may be used for TL termination and DCbiasing. In another example, although example embodiments describedhereinabove may have been described primarily with reference to awaveguide modulator device including an MZI, it will be appreciated thatprinciples and device configurations described hereinabove withreference to specific examples may be adopted to other types of opticalwaveguide modulators.

Furthermore, although some of the embodiment's described hereinabove useHSPMs in the form of depletion-mode p/n junctions formed insemiconductor waveguides, other embodiments may use forward-biased ornon-biased p/n junctions, or use electro-optic properties of thewaveguide arms material that do not require p/n junctions to modulatethe refractive index in a portion of the waveguide arm, and hence tomodulate the phase or amplitude of propagating light.

Furthermore in the description above, for purposes of explanation andnot limitation, specific details are set forth such as particulararchitectures, interfaces, techniques, etc. in order to provide athorough understanding of the present invention. In some instances,detailed descriptions of well-known devices, circuits, and methods areomitted so as not to obscure the description of the present inventionwith unnecessary detail. Thus, for example, it will be appreciated bythose skilled in the art that block diagrams herein can representconceptual views of illustrative circuitry embodying the principles ofthe technology. All statements herein reciting principles, aspects, andembodiments of the invention, as well as specific examples thereof, areintended to encompass both structural and functional equivalentsthereof. Additionally, it is intended that such equivalents include bothcurrently known equivalents as well as equivalents developed in thefuture, i.e., any elements developed that perform the same function,regardless of structure. Furthermore, it will be appreciated that eachof the example embodiments described hereinabove may include featuresdescribed with reference to other example embodiments.

Thus, while the present invention has been particularly shown anddescribed with reference to example embodiments as illustrated in thedrawing, it will be understood by one skilled in the art that variouschanges in detail may be affected therein without departing from thespirit and scope of the invention as defined by the claims.

1. An optical waveguide modulator comprising: an input optical port forreceiving input light; an output optical port for outputting modulatedlight; first and second waveguide arms extending optically in parallelbetween the input and output optical ports to guide the input light fromthe input optical port to the output optical port along two light paths;a plurality of p/n junctions comprising one or more first p/n junctionsformed in the first waveguide arm and one or more second p/n junctionsformed in the second waveguide arm, each p/n junction comprising ananode electrode and a cathode electrode; a first transmission line (TL)extending along the first and second waveguide arms and electricallycoupled to the anode electrode of each of the one or more first p/njunctions and to the cathode electrode of each of the one or more secondp/n junctions; and, a second transmission line (TL) extending along thefirst and second waveguide arms and electrically coupled to the cathodeelectrode of each of the one or more first p/n junctions and to theanode electrode of each of the one or more second p/n junctions; and adifferential driver configured to feed complementary electrical signalsinto the first and second transmission lines.
 2. The optical waveguidemodulator of claim 10, further comprising a differential driverconfigured to feed complementary electrical signals into the first andsecond transmission lines.
 3. The optical waveguide modulator of claim 1including electrical circuitry for providing a DC bias voltage to atleast one of the cathode electrode and the anode electrode of each p/njunction.
 4. An optical waveguide modulator comprising: an input opticalport for receiving input light; an output optical port for outputtingmodulated light; first and second waveguide arms extending optically inparallel between the input and output optical ports to guide the inputlight from the input optical port to the output optical port along twolight paths; a plurality of p/n junctions comprising one or more firstp/n junctions formed in the first waveguide arm and one or more secondp/n junctions formed in the second waveguide arm, each p/n junctioncomprising an anode electrode and a cathode electrode; a firsttransmission line (TL) extending along the first and second waveguidearms and electrically coupled to the anode electrode of each of the oneor more first p/n junctions and to the cathode electrode of each of theone or more second p/n junctions; and, a second transmission line (TL)extending along the first and second waveguide arms and electricallycoupled to the cathode electrode of each of the one or more first p/njunctions and to the anode electrode of each of the one or more secondp/n junctions; and electrical circuitry for providing a DC bias voltageto at least one of the cathode electrode and the anode electrode of eachp/n junction; wherein each of the cathode electrodes is AC-coupled toone of the first and second transmission lines, and each of the anodeelectrodes is either DC-coupled or AC coupled to one of the first andsecond transmission lines.
 5. The optical waveguide modulator of claim 4wherein the electrical circuitry includes one or more resistorselectrically connected to the cathode electrodes for DC biasing thereof.6. An optical waveguide modulator comprising: an input optical port forreceiving input light; an output optical port for outputting modulatedlight; first and second waveguide arms extending optically in parallelbetween the input and output optical ports to guide the input light fromthe input optical port to the output optical port along two light paths;a plurality of p/n junctions comprising one or more first p/n junctionsformed in the first waveguide arm and one or more second p/n junctionsformed in the second waveguide arm, each p/n junction comprising ananode electrode and a cathode electrode; a first transmission line (TL)extending along the first and second waveguide arms and electricallycoupled to the anode electrode of each of the one or more first p/njunctions and to the cathode electrode of each of the one or more secondp/n junctions; a second transmission line (TL) extending along the firstand second waveguide arms and electrically coupled to the cathodeelectrode of each of the one or more first p/n junctions and to theanode electrode of each of the one or more second p/n junctions; andelectrical circuitry for providing a DC bias voltage to at least one ofthe cathode electrode and the anode electrode of each p/n junction;wherein each of the anode electrodes is AC-coupled to one of the firstand second transmission line, and each of the cathode electrodes iseither DC-coupled or AC coupled to one of the first and secondtransmission lines.
 7. The optical waveguide modulator of claim 6wherein the electrical circuitry includes one or more resistorselectrically connected to the anode electrodes for DC biasing thereof.8. The optical waveguide modulator of claim 1 wherein the first andsecond transmission lines cross each other at least once forming a TLcrossing.
 9. The optical waveguide modulator of claim 8 wherein the oneor more first p/n junctions comprises two first p/n junctions ofopposite polarity disposed at opposite sides of the TL crossing, and theone or more second p/n junctions comprises two second p/n junctions ofopposite polarity disposed at opposite sides of the TL crossing.
 10. Anoptical waveguide modulator comprising: an input optical port forreceiving input light; an output optical port for outputting modulatedlight; first and second waveguide arms extending optically in parallelbetween the input and output optical ports to guide the input light fromthe input optical port to the output optical port along two light paths;a plurality of p/n junctions comprising one or more first p/n junctionsformed in the first waveguide arm and one or more second p/n junctionsformed in the second waveguide arm, each p/n junction comprising ananode electrode and a cathode electrode; a first transmission line (TL)extending along the first and second waveguide arms and electricallycoupled to the anode electrode of each of the one or more first p/njunctions and to the cathode electrode of each of the one or more secondp/n junctions; and, a second transmission line (TL) extending along thefirst and second waveguide arms and electrically coupled to the cathodeelectrode of each of the one or more first p/n junctions and to theanode electrode of each of the one or more second p/n junctions; andelectrical circuitry for providing a DC bias voltage to at least one ofthe cathode electrode and the anode electrode of each p/n junction;wherein the electrical circuitry includes one or more couplingelectrodes electrically connected to the cathode electrodes or the anodeelectrodes and capacitively coupled to one of the first and secondtransmission lines.
 11. The optical waveguide modulator of claim 10wherein the one or more coupling electrodes are disposed over or underthe first or second transmission lines with an insulating layertherebetween.
 12. The optical waveguide modulator of claim 10 whereineach of the first and second TL has an input end for receiving anelectrical drive signal, wherein one of the one or more couplingelectrodes extends along the first TL for at least a portion of a lengththereof, and wherein at least one of the cathode electrodes or the anodeelectrodes is electrically connected to the one of the one or morecoupling electrodes at a distal end thereof that is farther away fromthe input end of the first TL.
 13. The optical waveguide modulator ofclaim 10 wherein the one or more coupling electrodes are disposed nextto the first or second transmission lines coplanar therewith.
 14. Anoptical waveguide modulator comprising: an input optical port forreceiving input light; an output optical port for outputting modulatedlight; first and second waveguide arms extending optically in parallelbetween the input and output optical ports to guide the input light fromthe input optical port to the output optical port along two light paths;a first phase modulator (PM) disposed in the first waveguide arm andcomprising an anode electrode and a cathode electrode; a second PMdisposed in the second waveguide arm and comprising an anode electrodeand a cathode electrode, wherein each of the first and second PMs isconfigured to modulate a phase of light propagating therein in responseto a voltage applied between the anode and cathode electrodes thereof; afirst transmission line (TL) extending along the first and secondwaveguide arms and electrically coupled to the anode electrode of thefirst PM and the cathode electrode of the second PM; and, a second TLextending along the first and second waveguide arms and electricallycoupled to the cathode electrode of the first PM and to the anodeelectrode of the second PM.
 15. The waveguide modulator of claim 14wherein the first and second waveguide arms comprise electro-opticmaterial.
 16. The waveguide modulator of claim 14 wherein the first andsecond waveguide arms comprise semiconductor material, and wherein thefirst and second PMs each comprise a p/n junction.
 17. The waveguidemodulator of claim 16 wherein at least the anode electrodes of the firstand second PMs or at least the cathode electrodes of the first andsecond PMs are AC-coupled to the corresponding first or second TLs. 18.The waveguide modulator of claim 17 comprising a silicon photonics chipwherein the first and second waveguide arms and the first and second TLsare formed on the silicon photonics chip, and wherein the semiconductormaterial comprises silicon.
 19. The waveguide modulator of claim 16including first and second coupling electrodes disposed next to thefirst and second TLs respectively so as to be electrically AC coupledtherewith, and wherein either the anode electrodes or the cathodeelectrodes of the first and second PMs are electrically connected in DCto the first and second coupling electrodes respectively.
 20. Thewaveguide modulator of claim 19 wherein the first and second couplingelectrodes are disposed directly over or under the first and second TLsrespectively.